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Dark zone

This property can be applied to the detection of substances that absorb in the UV region For on layers containing a fluorescent indicator or impregnated with a fluorescent substance the emission is reduced in regions where UV-active compounds partially absorb the UV light with which they are irradiated. Such substances, therefore, appear as dark zones on a fluorescent background (Fig. 4A). [Pg.10]

The emission of the indicator is reduced in places where there are substance zones that absorb at 2 = 254 nm present in the chromatogram. This produces dark zones (Fig 4A), whose intensity (or rather lack of it) is dependent on the amount of substance applied. If the plate background is set to 100% emission the phosphorescence is reduced appropriately in the region of the substance zones. When the chromatogram is scanned peaks are produced, whose position with respect to the start can be used to calculate Rf values and whose area or height can be used to construct cahbration curves as a function of the amount applied (Fig. 25). [Pg.33]

Detection and result The chromatogram was freed from mobile phase in a stream of warm air, immersed in the reagent solution for 1 s and heated to 120°C for 20 min. Intense yellow to brown zones of various hues were produced these appeared as dark zones on a fluorescent background under long-wavelength UV light (X = 365 nm). [Pg.190]

Detection and result When viewed under short-wavelength UV light X = 254 nm) dark zones were visible due to fluorescence quenching. [Pg.96]

Brief exposure to nitrous fumes (up to 3 min) leaves the fluorescent power of the acid-instable fluorescence indicator 254. incorporated into most TLC layers, largely unaffected, so that the nitroaromatics so formed can be detected as dark zones on a green fluorescent background [1]. For purposes of in situ quantitation it is recommended that the fluorescence indicator be destroyed by 10 min exposure to nitrous fumes in order to avoid difficulties in the subsequent evaluation [1]. [Pg.172]

Bioluminescence can be used for spedfic detection of separated bioactive compounds on layers (BioTLC) [46]. After development and drying the mobile phase by evaporation, the layer is coated with microorganisms by immersion of the plate. Single bioactive substances in multicomponent samples are located as zones of differing luminescence. The choice of the luminescent cells determines the specificity of detection. A specific example is the use of the marine bacterium Vibrio fischeri with the BioTLC format. The bioluminescence of the bacteria cells on the layer is reduced by toxic substances, which are detected as dark zones on a fluorescent background. BioTLC kits are available from ChromaDex, Inc. (Santa Ana, CA). [Pg.183]

The inclusion of a fluorescent dye into thin-layer plates can be used to detect substances that quench its fluorescence and so result in dark zones when the chromatogram is examined under ultraviolet radiation. Autoradiography can also be used in thin-layer chromatography and electrophoresis when samples are radio-labelled. [Pg.97]

Further inspection of Fig. 4.5 demonstrates that the O atoms are surrounded by dark zones. The STM technique probes not only the atomic topography but also the electronic structure, and the dark zones reflect the modification of the local electronic density in the vicinity of the adsorbates, this modification being responsible for the operation of indirect interactions (which may be either repulsive or attractive) between adsorbed particles mediated through the substrate. [Pg.59]

Burned gases Luminous zone Dark zone... [Pg.152]

In Fig. 12 in Ref 25, fluorescence microscopy images of different dye-loaded zeolite L single crystals are shown. Each line consists of three pictures of the same sample, but with different polarizations of the fluorescence observed. In the first one, the total fluorescence of the crystals is shown, and in the others, the fluorescence with the polarization direction indicated by the arrows is displayed. The zeolite was loaded with the following dyes (A) Py+, (B) PyGY", (C) PyB +, (D) POPOP (see Table 1). Most crystals show a typical sandwich structure with fluorescent dyes at the crystal ends and a dark zone in the middle. This situation can be observed when the diffusion of the dyes in the channels has not yet reached its equilibrium situation. It illustrates nicely how the molecules penetrate the crystals via the two openings on each side of the one-dimensional channels. [Pg.333]

This reduction of NO is highly exothermic but relatively slow at low pressure, because it appears to be a third-order reaction, similar to the dark-zone reaction of nitropolymer combustion. The overall reaction of HNF is represented by... [Pg.127]

The combustion of H2, CO, and hydrocarbons with NO is important in both the dark zone and the flame zone of nitropolymer propellants. It is well known that NO behaves in a complex way in combustion processes, in that at certain concentrations it may catalyze a reaction to promote a process, while at other concentrations it may inhibit the reaction. Sawyer and GlassmanP attempted to estabUsh a measurable reaction between H2 and NO in a flow reactor at 0.1 MPa. Over a wide range of mixture ratios, they found that the reaction did not occur readily below the temperature of NO dissociation, except in the presence of some radicals. Mixtures of CO and NO are also difficult to ignite, and only mixtures rich in NO could be ignited at 1720 K. [Pg.130]

The combustion wave of a double-base propellant consists of the following five successive zones, as shovm in Fig. 6.3 (I) heat conduction zone, (II) soHd-phase reaction zone, (III) fizz zone, (IV) dark zone, and (V) flame zone-l i -i -i ]... [Pg.144]

IV) Dark zone In this zone, oxidation reactions of the products formed in the fizz-zone reaction take place. Nitric oxide, carbon monoxide, hydrogen, and carbonaceous fragments react to produce nitrogen, carbon dioxide, water, etc. These exothermic reactions occur only very slowly unless the temperature and/or pressure is sufficiently high. [Pg.145]

V) Flame zone When the dark-zone reactions occur rapidly after an induction period, they produce a flame zone in which the final combustion products are formed and attain a state of thermal equiUbrium. When the pressure is low, below about 1 MPa, no flame zone is produced because the reduction of nitric oxide is too slow to produce nitrogen. [Pg.145]

The soUd-phase reaction zone is also termed the subsurface reaction zone or condensed-phase reaction zone . As the dark zone reaction represents an induction zone ahead of the flame zone, the dark zone is also termed the preparation zone when it produces a luminous flame. Since the flame zone is luminous, it is also termed the luminous flame zone . [Pg.145]

The thermal structure of the combustion wave of a double-base propellant is revealed by its temperature profile trace. In the solid-phase reaction zone, the temperature increases rapidly from the initial temperature in the heat conduction zone, Tq, to the onset temperature of the solid-phase reaction, T , which is just below the burning surface temperature, T. The temperature continues to increase rapidly from T to the temperature at the end of the fizz zone, T, which is equal to the temperature at the beginning of the dark zone. In the dark zone, the temperature increases relatively slowly and the thickness of the dark zone is much greater than that of the solid-phase reaction zone or the fizz zone. Between the dark zone and the flame zone, the temperature increases rapidly once more and reaches the maximum flame temperature in the flame zone, i. e., the adiabatic flame temperature, Tg. [Pg.146]

Thus, the combustion wave structure of double-base propellants appears to showa two-stage gas-phase reaction, taking place in the fizz zone and the dark zone. The thickness of the fizz zone is actually dependent on the chemical kinetics of the... [Pg.146]


See other pages where Dark zone is mentioned: [Pg.176]    [Pg.77]    [Pg.240]    [Pg.16]    [Pg.449]    [Pg.98]    [Pg.143]    [Pg.150]    [Pg.49]    [Pg.50]    [Pg.51]    [Pg.172]    [Pg.192]    [Pg.129]    [Pg.391]    [Pg.542]    [Pg.833]    [Pg.878]    [Pg.5]    [Pg.180]    [Pg.182]    [Pg.32]    [Pg.236]    [Pg.17]    [Pg.151]    [Pg.145]    [Pg.146]    [Pg.147]   
See also in sourсe #XX -- [ Pg.144 , Pg.160 , Pg.171 , Pg.176 , Pg.205 , Pg.235 , Pg.243 , Pg.252 , Pg.345 , Pg.374 ]

See also in sourсe #XX -- [ Pg.144 , Pg.160 , Pg.171 , Pg.176 , Pg.205 , Pg.235 , Pg.243 , Pg.252 , Pg.345 , Pg.374 ]

See also in sourсe #XX -- [ Pg.125 , Pg.171 , Pg.183 , Pg.215 ]




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Dark zone index

Dark zone length

Dark zone of double-base propellant

Dark zone reaction

Dark zone temperature

Dark zone velocity

Pressure exponent of the dark zone

Reaction Mechanism in the Dark Zone

Reaction time in the dark zone

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